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Longitudinal Bending Stress Stress at saddles in ts 1 in A 40 Q 25000 lb R 50 in K1 0.33 H 50 in L 100 in P 250 Ps α Ro A = 40 in b = 24 in L = 1000 in Do = 100 in H α = 120 o E = 85 % S = 17500 Psi (material SA- 516, grade 65, 620 o F W operation = 500.000 lb Q = lb

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Page 1: tugas res

Longitudinal Bending Stress

Stress at saddles

in ts 1 inA 40 Q 250000 lb

R 50 inK1 0.335

H 50 inL 1000 in

P 250 Psi

α

Ro

A = 40 in b = 24 in

L = 1000 in

Do = 100 in

H

α = 120o

E = 85 %

S = 17500 Psi (material SA-516, grade 65,

620 oF

Woperation = 500.000 lb

Q = lb

Page 2: tugas res

Stress at midspan

S1

Q A 11

AL

R2 H22 A L

14 H3 L

K1 R2 ts

S1 1.47 103 Psi

S1

Q L4

12 R2 H2

L2

14 H3 L

4 AL

3.14R2 ts

S1 7.619 103 Psi

Page 3: tugas res

Based upon our calculation, the stress at midspan is higher than the stress at saddles, it

results tension at the bottom and compression at the top.This is the following profile

resulting the higher midspan stress :

Stress due to internal pressure

Stress value of girth seam

Sum of tension

S1 + S2 = 15310 psi

S2P R2 ts

S2 7.692 103 Psi

Psi

Page 4: tugas res

For A = 40 in, we found that the sum of tension is higher than the stress value of girth

seam, it means that the vessel will collapse, or on the other words the value of A is still

not satisfactory.

We have to make some of trial and error to find the exact value of A.

Assume the value of A = 96 in

Stress at saddles

Stress at midspan

S1

Q A 11

AL

R2 H22 A L

14 H3 L

K1 R2 ts

S1 5.379 103 Psi

S1

Q L4

12 R2 H2

L2

14 H3 L

4 AL

3.14R2 ts

S1 5.424 103 Psi

Page 5: tugas res

Sum of tension

S1 + S2 = 13116 psi

The sum of tension doesn’t exceed the stress value of the girth seam. The value of A is

already satisfactory.

Tangential Shear Stress (S2)

Sice A (96) > R/2 (50/2), the applicable formula :

S2 doesn’t exceed the stress value of shell material multiplied by 0.8 ; 0.8* 15500

= 12400 psi

Circumferential Stress

S2K2 QR ts

L 2 A

L43

H

S2 5.459 103

Psi

Page 6: tugas res

Stress at the horn of saddle (S4)

Since L (1000) > 8.R (400), A (96) > R/2 (50/2)the applicable formula :

For the value of b = 24 in, S4 exceeds the stress value of shell material multiply by 1.5 ;

17500x1.5 = 26250 psi. the value of b is not satisfactory.

Assume that the value of b = 60 in. the value of S4 will be :

Since S4 doesn’t exceed the stress value of shell material multiply by 1.5, thus the value

of b = 60 in is already satisfactory.

Stress at bottom of shell (S5)

; where K7 = 0.76 ; yield point = 35000 psi (page :

147 ).

S4Q

4.ts b 1.56 R ts( )

3 K6 Q2 ts

S4 2.673 104

S4Q

4.ts b 1.56 R ts( )

3 K6 Q2 ts

S4 2.556 104

S5K7 Q

ts b 1.56 R ts( )

S5 3.343 103

Psi

psi

Page 7: tugas res

S5 doesn’t exceed the compression yield multiplied by 0.5 ; 35000x 0.5

= 17500 psi.